A Charged Isolated Conductor — Question 9

Section 23-5 · Physics pages 3728–3729

Question 9 Connected unequal spheres share charge but not equal surface fields Two conducting spheres of radii R and 3R are joined by a thin wire and separated by a distance much larger than either radius. Their total charge is +8.00 nC. Neglect mutual distortion and wire charge. Use the supplied equilibrium relation Q1/R1 = Q2/R2. R 3R Schematic connection; actual separation is assumed much larger than both radii. (a) Find the final charges and their uniform surface charge densities in terms of R. (b) Compare the surface fields. If the same field limit applies to both spheres, identify which sphere reaches it first as total charge is increased.
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Question 9 - Solution Connected unequal spheres share charge but not equal surface fields R 3R (a) Method and calculation Q2 = 3Q1, Q1 + Q2 = 8.00 nC ⇒Q1 = 2.00, Q2 = 6.00 (nC). σ1 = 2.00 nC 4πR2 , σ2 = 6.00 nC 36πR2 . (b) Interpretation and further calculation Ei = σi/ϵ0, E1 E2 = Q1/R2 Q2/(9R2) = 3. E1 = 3E2 ⇒the smaller sphere reaches the common limit first. The supplied sharing relation is an additional equilibrium condition; charge conservation and Gauss law alone do not determine the partition. Physical check The approximation explicitly excludes the strong surface distortion that would occur if the spheres were close together.

Question 9

Connected unequal spheres share charge but not equal surface fields

Two conducting spheres of radii R and 3R are joined by a thin wire and separated by a distance much larger than either radius. Their total charge is +8.00+8.00 nC. Neglect mutual distortion and wire charge. Use the supplied equilibrium relation Q1/R1=Q2/R2Q_1/R_1=Q_2/R_2.

Diagram shown in the original SVG worksheet.

  1. Find the final charges and their uniform surface charge densities in terms of R.

  2. Compare the surface fields. If the same field limit applies to both spheres, identify which sphere reaches it first as total charge is increased.

Question 9 - Solution

Connected unequal spheres share charge but not equal surface fields

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Q2=3Q1,Q1+Q2=8.00nC⇒Q1=2.00,Q2=6.00(nC).Q_2=3Q_1,\quad Q_1+Q_2=8.00\,\mathrm{nC}\Rightarrow Q_1=2.00,\ Q_2=6.00\quad(\mathrm{nC}).σ1=2.00nC4πR2,σ2=6.00nC36πR2.\sigma_1=\frac{2.00\,\mathrm{nC}}{4\pi R^2},\quad\sigma_2=\frac{6.00\,\mathrm{nC}}{36\pi R^2}.

(b) Interpretation and further calculation

Ei=σi/ϵ0,E1E2=Q1/R2Q2/(9R2)=3.E_i=\sigma_i/\epsilon_0,\quad\frac{E_1}{E_2}=\frac{Q_1/R^2}{Q_2/(9R^2)}=3.E1=3E2⇒the smaller sphere reaches the common limit first.E_1=3E_2\Rightarrow\text{the smaller sphere reaches the common limit first}.The supplied sharing relation is an additional equilibrium condition; charge conservation and Gauss law alone do not determine the partition.

Physical check

The approximation explicitly excludes the strong surface distortion that would occur if the spheres were close together.